Ag. Bashkirov et Av. Vityazev, STATISTICAL-MECHANICS OF FRAGMENTATION PROCESSES OF ICE AND ROCK BODIES, Planetary and space science, 44(9), 1996, pp. 909-915
It is a well-known experimental fact that impact fragmentation, specif
ically of ice and rock bodies, causes a two-step (''knee''-shaped) pow
er distribution of fragment masses with exponent values within the lim
its -4 and -1.5 (here and henceforth the differential distribution is
borne in mind). A new theoretical approach is proposed to determine th
e exponent values, a minimal fracture mass, and properities of the kne
e. As a basis for construction of nonequilibrium statistical mechanics
of condensed matter fragmentation the maximum-entropy variational pri
nciple is used. In contrast to the usual approach founded on the Boltz
mann entropy the more general Tsallis entropy allowing stationary solu
tions not only in the exponential Boltzmann-Gibbs form but in the form
of the power (fractal) law distribution as well is invoked. Relying o
n the analysis of a lot of published experiments a parameter beta is i
ntroduced to describe an inhomogeneous distribution of the impact ener
gy over the target. It varies from 0 (for an utterly inhomogeneous dis
tribution of the impact energy) to 1 (for a homogeneous distribution).
The lower limit of fragment masses is defined as a characteristic fra
gment mass for which the energy of fragment formation is minimal. This
mass value depends crucially on the value of beta. It is shown that f
or beta much less than 1 only small fragment can be formed, and the ma
ximal permitted fragment (of mass m(1)) is the upper boundary of the f
irst stage of the fracture process and the point where the knee takes
place. The second stage may be realized after a homogeneous redistribu
tion of the remainder of the impact energy over the remainder of the t
arget (when beta --> 1). Here, the formation of great fragments is per
mitted only and the smallest of them (of mass m(2)) determines a lower
boundary of the second stage. Different forms of the knee can be obse
rved depending on relations between m(1) and m(2). Copyright (C) 1996
Elsevier Science Ltd